Journal
EUROPHYSICS LETTERS
Volume 70, Issue 4, Pages 492-498Publisher
EDP SCIENCES S A
DOI: 10.1209/epl/i2005-10020-8
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The Tomonaga-Luttinger parameter K. determines the critical behavior in quasi-one-dimensional correlated electron systems, e. g., the exponent a for the density of states near the Fermi energy. We use the numerical density-matrix renormalization group method to calculate K. from the slope of the density-density correlation function in momentum space at zero wave vector. We check the accuracy of our new approach against exact results for the Hubbard and XXZ Heisenberg models. We determine K. in the phase diagram of the extended Hubbard model at quarter filling, nc = 1/2, and confirm the bosonization results K-rho = n(c)(2) = 1/4 on the critical line and K-rho(CDW). = n(c)(2)/2 = 1/8 at infinitesimal doping of the charge-density-wave (CDW) insulator for all interaction strengths. The doped CDW insulator exhibits exponents alpha > 1 only for small doping and strong correlations.
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